WO2016086504A1 - 一种两相流体回路真空热性能试验装置及方法 - Google Patents
一种两相流体回路真空热性能试验装置及方法 Download PDFInfo
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- WO2016086504A1 WO2016086504A1 PCT/CN2015/000834 CN2015000834W WO2016086504A1 WO 2016086504 A1 WO2016086504 A1 WO 2016086504A1 CN 2015000834 W CN2015000834 W CN 2015000834W WO 2016086504 A1 WO2016086504 A1 WO 2016086504A1
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- temperature
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- heat
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Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
- F28D15/00—Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies
- F28D15/02—Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies in which the medium condenses and evaporates, e.g. heat pipes
- F28D15/0266—Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies in which the medium condenses and evaporates, e.g. heat pipes with separate evaporating and condensing chambers connected by at least one conduit; Loop-type heat pipes; with multiple or common evaporating or condensing chambers
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N25/00—Investigating or analyzing materials by the use of thermal means
- G01N25/20—Investigating or analyzing materials by the use of thermal means by investigating the development of heat, i.e. calorimetry, e.g. by measuring specific heat, by measuring thermal conductivity
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28F—DETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
- F28F2200/00—Prediction; Simulation; Testing
- F28F2200/005—Testing heat pipes
Definitions
- the invention relates to a spacecraft thermal control technology leading city, in particular to a two-phase fluid circuit vacuum thermal performance testing device and method. Background technique
- the two-phase fluid circuit technology is a spacecraft thermal control technology that has been developed at home and abroad for nearly two decades, mainly including loop heat pipe technology, mechanical pump-driven two-phase fluid circuit technology, and gravity-driven two-phase fluid circuit technology.
- the gravity-driven two-phase fluid loop system is the key technology to solve the moonlight night of the patrol and lander in the lunar exploration project.
- the two-phase fluid loop system is used to bring the heat of the isotope heat source into the load compartment to ensure the equipment of the load compartment. The temperature is not too low.
- the system composition of the gravity driven two-phase fluid circuit is shown in Figure 1, including the evaporator 1 (including the wire mesh evaporator 7, the liquid flow divider 8 and the vapor manifold 9), the vapor line 2, the condensation line 3, and the liquid storage. 4, a liquid line 6 and a control valve 5, wherein the condensing line 3 is located above the gravity field of the accumulator 4, the evaporator 1 is located below the gravity field of the accumulator 4, and is coupled with the isotope heat source, the accumulator 4 a gravity assisted height difference is formed between the inner liquid surface and the bottom of the evaporator 1; the liquid accumulator 4 is connected to the inlet of the evaporator 1 through the liquid line 6, and the control valve 5 is provided on the liquid line 6, and the outlet of the evaporator 1 is in turn It is connected to the accumulator 4 via a vapor line 2, a condensing line 3, to form a closed piping system.
- the gravity-driven two-phase fluid circuit has good heat transfer characteristics in the temperature range of -50 ° C to 7 (TC temperature, ammonia is selected as the working medium.
- TC temperature -50 ° C to 7
- ammonia is selected as the working medium.
- the gravity-driven two-phase fluid circuit control valve 5 is opened, and the gravity drive is started.
- the two-phase fluid circuit introduces the heat of the isotope nuclear heat source into the interior of the detector.
- the gravity-driven two-phase fluid circuit control valve 5 is closed, the gravity-driven two-phase fluid circuit is closed, and the isotope nuclear heat source is blocked from transmitting heat to the detector. .
- the gravity-driven two-phase fluid circuit can transmit the heat transfer amount required by the system at the moon-night, and the gravity-driven two-phase fluid circuit system can be normally blocked at the time of the moon.
- the gravity-driven two-phase fluid circuit must be vacuum tested, and the gravity-driven two-phase fluid circuit is required to drive the steady-state heat transfer of the two-phase fluid circuit at a given steady-state operating temperature (ie, the temperature of the accumulator 4).
- the steady-state heat transfer temperature difference (the temperature difference between the evaporator 1 and the accumulator 4) satisfies the specifications.
- the present invention provides a two-phase fluid circuit vacuum thermal performance testing device, which can test and evaluate the heat transfer capability and blocking performance of a two-phase fluid circuit at different operating temperatures.
- the present invention is implemented as follows:
- the two-phase fluid circuit vacuum thermal performance test device comprises: a heat sink, a temperature control heater, a multi-layer heat insulation component, a temperature sensor, a simulated heat source and a circuit bracket; wherein the heat sink is thermally insulated and installed on the upper part of the circuit bracket through the heat insulation pad
- the condensation line of the two-phase fluid circuit is buried in the heat dissipation plate, and the reservoir of the two-phase fluid circuit is half buried in the heat dissipation plate;
- the evaporator in the two-phase fluid circuit is insulated and installed in the lower part of the circuit support;
- the device is installed in the steam line, the accumulator, the control valve and the liquid line of the two-phase fluid circuit;
- the temperature sensor is installed in the evaporator of the two-phase fluid circuit, the steam line, the condensing line, the accumulator, the control valve and Liquid piping, simulated heat source, and edge area of the heat sink; multi-layer insulation assembly wrapped in steam The pipeline,
- the evaporator is mounted on the heat insulation board, and the analog heat source is placed inside the evaporator, and the ear piece of the simulation heat source tool is fixed on the heat insulation board by the screw and the heat insulation pad, and the heat insulation board passes through 4 partitions.
- the hot column is fixedly mounted on the circuit bracket;
- the analog heat source is used to control the temperature of the evaporator so that the temperature of the evaporator is -55 ° C ⁇ 50 ° C;
- the heat sink heater is used to control the temperature of the heat sink, so that the temperature of the heat sink is -60 ° C ⁇ 50 ° C
- the temperature control heater is used to prevent the steam line, the accumulator, the control valve and the liquid line from freezing, and the self-control threshold of the temperature control heater is set to -55 ° C ⁇ -30 ° C;
- the temperature sensor is used to observe the state of the ammonia working fluid in the two-phase fluid circuit in the components, and the temperature sensor is installed at:
- At least two temperature sensors are arranged on the four fins of the evaporator in the height direction, one of which is located at the lower end of the evaporator fin and one of which is located at the upper end of the evaporator fin;
- One temperature sensor is arranged at the inlet, the top and the outlet of the steam line;
- a temperature sensor is arranged at the inlet and the outlet of the condensing line, and at least one temperature sensor is arranged on the fin of the condensing line;
- the outer surface of the accumulator is arranged with three temperature sensors in the height direction, which are respectively located in the air space of the accumulator, the gas-liquid interface and the liquid space;
- At least one temperature sensor is disposed on the liquid line connecting the accumulator and the control valve, and at least one temperature sensor is disposed on the liquid line connecting the control valve and the evaporator;
- a temperature sensor is arranged on the control valve; Arranging at least one temperature sensor on the analog heat source;
- At least one temperature sensor is disposed in an edge region of the inner surface of the heat dissipation plate.
- the heat insulating plate (12), the heat insulating pad (13) and the heat insulating column (14) are made of polyimide or glass steel.
- the substrate of the heat dissipation plate (11) is an aluminum plate or a honeycomb plate, and the surface of the heat dissipation plate (11) is pasted with an OSR sheet or a coating with a high emissivity.
- the temperature control heater is a heating sheet, a heating wire, a heating belt or a heating plate.
- the invention also provides a two-phase fluid circuit vacuum thermal performance test method using the above test device, which can test and evaluate the heat transfer capacity and the blocking performance of the two-phase fluid circuit at different working temperatures.
- the test method includes the following steps:
- Step 2 Place the circuit bracket into the vacuum chamber and evacuate it so that the vacuum is less than 2x l (T 3 Pa, set the temperature control heater on the accumulator, control valve, liquid line and steam line to be self-controlled.
- the self-control threshold is -55° (: ⁇ -30 °C; the self-control threshold for setting the heat sink heater is -55 °C ⁇ -30 °C;
- Step 3 through the heat sink of the vacuum chamber, the liquid nitrogen is lowered to lower the temperature of the vacuum chamber to -150 ° C; the temperature of the liquid storage device is lowered to the first test temperature -50 ° C, and the two-phase fluid circuit working condition is balanced;
- the balance of the working condition is that the temperature of the accumulator remains unchanged for half an hour or the monotonic change is less than 1 °C/h; the temperature of the accumulator is the operating temperature of the two-phase fluid circuit;
- the analog heat source increase the heating power of the analog heat source according to the set step size, reduce the heating power of the heat sink heater while increasing the heating power of the simulated heat source, and maintain the temperature of the liquid reservoir at -50 °C. And the balance of the two-phase fluid circuit condition is reached until the heating power of the heat sink heater is zero or the temperature of the evaporator rises to prevent the balance of the working condition; the heating power of the heat sink heater is The heating power of the simulated heat source at zero hour or the temperature of the evaporator rises before the equilibrium moment is the ultimate heat transfer capacity of the two-phase fluid circuit at the working temperature;
- Step 5 By reducing the power of the evaporator and increasing the power of the heat sink, changing the temperature of the liquid reservoir to each test temperature, according to the method of step 4, obtaining the ultimate heat transfer capability of the two-phase fluid circuit at each test temperature, wherein , changing the temperature of the reservoir in a step-up manner;
- the control valve is switched to check the blocking performance of the two-phase fluid circuit: After the valve is controlled, the temperature of the evaporator rises continuously and the temperature of the heat sink rises continuously. After the control valve is reopened, the temperature of the evaporator decreases and the temperature of the heat sink rises until the balance of the working condition is reached, indicating that the two-phase fluid circuit The blocking performance is normal; if the temperature of the evaporator does not change or rises steadily after the control valve is closed, it indicates that the blocking performance of the two-phase fluid circuit is abnormal.
- the analog heat source is turned on, so that the two-phase fluid circuit operates to accelerate the cooling rate of the evaporator.
- test device and the test method of the present invention can comprehensively and effectively evaluate the heat transfer and blocking performance of the two-phase fluid in a vacuum environment.
- the substrate of the heat sink is selected as an aluminum plate or a honeycomb plate. Applying an OSR sheet or spraying a high-emitting coating on the surface of the heat sink is beneficial to improving the heat dissipation rate of the heat sink.
- the temperature sensor is arranged to observe the state of the ammonia working fluid in the two-phase fluid circuit, to see if the components in the two-phase fluid circuit meet the temperature requirements, and to check whether the two-phase fluid circuit reaches equilibrium.
- the analog heat source is increased during the cooling process.
- the heating power can increase the temperature of the evaporator, and the ammonia working fluid in the two-phase fluid circuit transfers the heat of the evaporator to the condensing line, which can increase the cooling rate of the evaporator.
- Figure 1 is a schematic diagram of the composition of a gravity-driven two-phase fluid loop system.
- Figure 2 is a schematic diagram of a two-phase fluid circuit vacuum thermal performance test device.
- Figure 3 is a schematic view showing the installation of a two-phase fluid circuit evaporator.
- Figure 4 is a schematic view showing the arrangement of temperature sensors on a two-phase fluid circuit.
- Figure 5 shows the layout of the temperature sensor on the heat sink (including the condensing line).
- the present invention provides a two-phase fluid circuit vacuum thermal performance testing device, as shown in Fig. 2, comprising a heat sink 1 1 , a temperature control heater, a multilayer insulation assembly, a temperature sensor, a simulated heat source 15 and a circuit holder 17 .
- the two-phase fluid circuit and the heat dissipation plate 1 1 are heat-insulated on the circuit bracket 17, and the heat dissipation plate 1 1 is thermally insulated and installed on the upper part of the circuit bracket , for simulating the heat dissipation portion of the two-phase fluid circuit in the rail
- the condensing line 3 of the two-phase fluid circuit is buried in the heat dissipating plate 11, and the accumulator 4 of the two-phase fluid circuit is half buried in the heat dissipating plate 1 1 at the outlet of the condensing line 3;
- Evaporator 1 insulated installation In the lower part of the circuit support 17, located below the condensing line 3;
- the temperature control heater is installed in the steam line 2, the liquid reservoir 4, the control valve 5 and the liquid line 6 of the two-phase fluid circuit to prevent the pipeline from freezing
- the temperature sensor is installed in the evaporator 1, the steam line 2, the condensing line 3, the accumulator 4, the control valve 5 and the liquid line 6 of the two
- the substrate of the heat dissipation plate may be made of a material having better thermal conductivity such as an aluminum plate or a honeycomb plate, and an OSR sheet is attached to the outer surface thereof, or a coating with a high emissivity is sprayed, thereby facilitating heat dissipation.
- the heat insulation between the evaporator 1, the analog heat source 15 and the circuit support 17 is as shown in Fig. 3.
- the evaporator 1 is mounted on the heat shield 12, and the simulated heat source 15 is placed inside the evaporator 1, simulating the heat source 15 tooling.
- the tabs are fixed to the heat shield 12 by screws and a heat insulating mat 12 which is fixedly mounted on the circuit bracket 17 by means of four heat insulating columns 14.
- the heat insulating plate 12, the heat insulating pad 13 and the heat insulating column 14 are made of a material having a low thermal conductivity such as polyimide or glass reinforced plastic.
- the distance between the lower surface of the liquid diverter 8 and the upper surface of the heat shield 12 is greater than 10 mm, the effective insulation distance between the heat shield 12 and the circuit support 17 is greater than 100 mm, and the outer diameter of the heat shield 13 is less than 10 mm.
- the temperature sensor is a thermocouple temperature sensor, and its arrangement is shown in Figure 4. Place 34 temperature sensors on the two-phase fluid circuit:
- thermosensor 1 On the four fins of the evaporator 1, three temperature sensors are arranged uniformly from the bottom to the top in the height direction, a total of 12, numbered T1 ⁇ T12, and the sensing can be arranged only at the lower end and the upper end of the evaporator fins.
- the main purpose is to measure the temperature of the liquid working medium and the gaseous working in the evaporator, thereby reacting the working state of the evaporator 1.
- the condensing line 3 Arrange 9 temperature sensors on the inlet, outlet and condensation lines of the condensate line 3, number T16-T24, as shown in Figure 5; the condensing line 3 is generally equipped with fins for increasing the heat dissipation area, temperature The sensor is typically mounted on a fin.
- Three temperature sensors are arranged in the height direction on the outer surface of the accumulator 4 for measuring the temperature of the gas, gas-liquid interface and liquid in the accumulator 4.
- the liquid line 6 is divided into two sections, one section connecting the reservoir 3 and the control valve 5, and the other section connecting the control valve 5 and the evaporator 1.
- a temperature sensor number ⁇ 28
- a temperature sensor is arranged at a midpoint of the liquid line connecting the accumulator 3 and the control valve 5; and respectively arranged at the inlet and the outlet of the liquid line connecting the control valve 5 and the evaporator 1
- One temperature sensor, numbered T31 and ⁇ 32 can also be arranged at the midpoint of the liquid line connecting the control valve 5 and the evaporator 1.
- control valve 5 consists of two parallel valves (a valve and b valve), a temperature sensor is arranged on the a valve and the b valve, respectively, numbered T29 and T30;
- the position of the temperature sensor is the position of the measuring point.
- the temperature control heater can be a heating plate, a heating wire, a heating belt, a heating plate or other heating method, and adopts PID control or on-off temperature control, mainly to prevent components of the two-phase fluid circuit from being frozen.
- the temperature control heater on the accumulator 4 is realized by installing two heating sheets in series on the accumulator 4; the control valve 5
- the upper temperature control heater is installed with a heating belt on the liquid pipeline connected to the control valve 5, as shown in Fig.
- the upper temperature control heater is realized by installing a heating belt between the measuring point 31 on the liquid line 6 and the measuring point 32; the temperature control heater on the steam line 2 is realized by three heating belts installed in series. .
- the temperature control heaters on the reservoir 4, control valve 5, liquid line 6 and vapor line 2 act primarily to prevent freezing of the line.
- the temperature control of the evaporator 1 is achieved by means of an analog heat source 15 installed inside it. Since the heat of the isotope heat source is transferred away by the two-phase fluid circuit during heat transfer, the temperature of the surface of the isotope heat source itself is reduced to match the temperature of the evaporator.
- the condensing line 2 is pre-buried in the heat dissipating plate 1 1 , which is substantially the same as the temperature of the heat dissipating plate 1 1 , and the temperature control of the heat dissipating plate 11 is controlled by the infrared heater 16 installed on the outer side of the heat dissipating plate 1 or pasted on the heat dissipating plate.
- the heater chip is realized.
- the temperature of the heat radiating plate 11 is controlled to be -60 ° C to 50 ° C. Due to the heat transfer of the ammonia working fluid during the operation of the two-phase fluid circuit, the temperatures of the evaporator 1, the steam line 2, the condensing line 3, the accumulator 4, the control valve 5 and the liquid line 6 are substantially at -55°. C ⁇ 50 ° (: range. Among them, the temperature of the reservoir 4 is the operating temperature of the two-phase fluid circuit.
- Select measuring point T1 (lower part of evaporator 1, near the outlet of liquid line 6), T3 (upper part of evaporator 1, near the inlet of vapor line 2), T14 (middle of vapor line 2), T17 (condensing line 3) Inlet), T23 (condensation line 3 outlet), T25 (upper reservoir 4, ie reservoir gas space), T27 (lower reservoir), T29-T30 (control valve a and control valve b), T3 1 (liquid line 6 inlet), T35-T38 (4 corners of heat sink 11) are temperature monitoring points, monitor whether the analog heat source 15, the heat sink 11 and the two-phase fluid circuit meet the temperature requirements, and at the same time, Compare the temperature of the temperature monitoring point with the other measuring points to determine whether the balance is reached.
- the vacuum heat performance test of the gravity-driven two-phase fluid circuit was carried out by using the above test device, and the ultimate heat transfer performance and blocking performance of the gravity-driven two-phase fluid circuit at different working temperatures were tested.
- the operating temperature of the two-phase fluid circuit is the temperature of the accumulator 4, and during the test, the temperature of the accumulator 4 is changed by changing the temperature of the evaporator 1 and the heat dissipating plate 11, the accumulator 4, the control valve 5, the liquid
- the temperature control heaters on line 6 and vapor line 2 are only used to prevent components in the two-phase fluid circuit from being frozen.
- the specific implementation steps are as follows:
- Step 1 the circuit 17 into a vacuum cartridge holder 10, a vacuum (degree of vacuum less than 2xl0_ 3 pa), the liquid reservoir 4 is provided, the control valve 5, the liquid conduit 6 and the vapor line temperature control heater 2
- the self-control threshold is -55 ° C ⁇ - 30 ° C, that is, when the temperature is lower than the self-control threshold, the temperature control heater is automatically turned on to prevent it from being frozen.
- Set the self-control threshold of the heat sink heater to -55 ° C - 30t.
- Step 2 Pass the liquid nitrogen to the heat sink of the vacuum chamber, reduce the vacuum chamber temperature to -150 °C, due to the steam line (2), the reservoir (4), the control valve (5) and the liquid of the two-phase fluid circuit.
- the pipeline (6) is wrapped by a multi-layer insulation component, and the cooling rate is slow, and the cooling plate has the fastest cooling rate.
- the simulated heat source 15 is turned on, so that two The phase fluid circuit operates, and the evaporator and the liquid reservoir are cooled by the condensing line in the heat dissipation plate to accelerate the cooling rate of the evaporator until the temperature of the liquid storage device is lowered to -50 ° C, when the temperature of the liquid storage device is half
- the temperature of the reservoir is the operating temperature of the two-phase fluid circuit.
- Step 3 Limit heat transfer capacity test: Increase the heating power of the evaporator according to a certain step size (ie, the heating power of the simulated heat source), and simultaneously reduce the heating power of the heat sink heater while increasing the heating power of the analog heat source.
- a certain step size ie, the heating power of the simulated heat source
- the heating power of the heat sink heater is zero or the temperature of the evaporator rises. Unable to maintain working condition balance.
- the heat sink heating power is 0, the heat sink reaches this work. The maximum heat dissipation at temperature, the continued increase in evaporator heating power will cause the temperature of the reservoir to rise and cannot be maintained at -50 °C.
- the heating power of the evaporator When the heating power of the evaporator is greater than the ultimate heat transfer capacity of the two-phase fluid circuit, the liquid in the evaporator is dried, causing the temperature of the evaporator to rise. Therefore, when the heating power of the heat sink heater is zero or the temperature of the evaporator rises, the heating power of the evaporator at the equilibrium moment is the ultimate heat transfer capacity of the two-phase fluid circuit at the operating temperature.
- Step 4 By reducing the power of the evaporator and increasing the power of the heat sink, changing the temperature of the reservoir, according to the method of step 3, the ultimate heat transfer capability of the two-phase fluid circuit at different working temperatures is obtained.
- the adjustment method of the working temperature is gradually increased, such as first measuring the ultimate heat transfer capacity at the operating temperature of -50 ° C, and then measuring -40 °C, -30°C, -20°C... ultimate heat transfer capacity at operating temperature.
- Blocking performance If the temperature of the evaporator rises and rises rapidly after the control valve is closed, the temperature of the heat sink is continuously lowered, the control valve is re-opened, the temperature of the evaporator is lowered, and the temperature of the heat sink is raised until the working condition is balanced. It indicates that the blocking performance of the two-phase fluid circuit is normal; if the temperature of the evaporator does not change or rises slowly after the control valve is closed, it indicates that the blocking performance of the two-phase fluid circuit is abnormal.
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Abstract
提供一种两相流体回路真空热性能试验装置及试验方法,能够对两相流体回路在不同工作温度下的传热能力和阻断性能进行测试和评估。所述试验装置包括散热板(11)、控温加热器、多层隔热组件、温度传感器、模拟热源(15)和回路支架(17),通过控制蒸发器(1)温度和散热板(11)温度改变两相流体回路的工作温度,设计试验方法,对重力驱动两相流体回路真空热性能进行传热、阻断能力试验,其中,温度传感器的布置有利于观察两相流体回路中氨工质的状态,查看两相流体回路中的各部件是否满足温度要求,同时还可以查看两相流体回路是否达到平衡。
Description
一种两相流体回路真空热性能试验装置及方法
技术领域
本发明涉及航天器热控制技术领城, 尤其涉及一种两相流体回路真空热性 能试验装置及方法。 背景技术
两相流体回路技术是近二十年来国内外重点发展的航天器热控制技术, 主 要包括环路热管技术、 机械泵驱动两相流体回路技术、 重力驱动两相流体回路 技术等。 重力驱动两相流体回路系统是解决嫦娥探月工程中巡视器和着陆器度 过月夜的关键技术, 通过两相流体回路系统, 将同位素热源的热量带入到载荷 舱内, 保证载荷舱各设备的温度不至于过低。 重力驱动两相流体回路的系统组 成如图 1所示, 包括蒸发器 1 (包括丝网蒸发器 7、 液体分流器 8和蒸气汇流器 9)、 蒸气管路 2、 冷凝管路 3、 储液器 4、 液体管路 6和控制阀 5 , 其中, 冷凝 管路 3位于储液器 4重力场上方, 蒸发器 1位于储液器 4重力场的下方、 并与 同位素热源耦合安装, 储液器 4 内液面和蒸发器 1 底部之间形成重力辅助高度 差; 储液器 4通过液体管路 6连接至蒸发器 1 入口, 在液体管路 6上设有控制 阀 5 , 蒸发器 1 出口依次通过蒸气管路 2、 冷凝管路 3连接至储液器 4 , 形成封 闭的管路系统。为确保重力驱动两相流体回路在 -50°C〜7(TC温度范围内具有良好 的传热特性, 选择氨作为工作介质。 月夜期间, 重力驱动两相流体回路控制阀 5 开启, 启动重力驱动两相流体回路, 将同位素核热源的热量引入探测器内部。 月昼期间, 重力驱动两相流体回路控制阀 5关闭, 关闭重力驱动两相流体回路, 阻断同位素核热源向探测器内部传递热源。
为了保证重力驱动两相流体回路技术能够正常运行, 同时保证在月夜时重 力驱动两相流体回路能够传递满足系统所需要的传热量、 在月昼时重力驱动两 相流体回路系统能够正常阻断, 必须对重力驱动两相流体回路进行真空试睑, 要求重力驱动两相流体回路在给定的稳态工作温度 (即储液器 4 温度) 下, 重 力驱动两相流体回路的稳态传热量和稳态传热温差 (蒸发器 1 与储液器 4之间 的温差) 满足技术指标。
由于重力驱动两相流体回路技术是航天器热控制的新型热控方法, 没有固 定的测试方式和测试方法。 同时, 考虑到月球恶劣的环境, 重力驱动两相流体 回路与同位素热源联合使用, 此种情况下的传热能力、 阻断性能的测试方法未 见文献报道, 需要自行摸索, 从而指导重力驱动两相流体回路的在轨应用。 发明内容
有鉴于此, 本发明提供了一种两相流体回路真空热性能试验装置, 采用该 装置, 能够对两相流体回路在不同工作温度下的传热能力和阻断性能进行测试、 评估。
为了解决上述技术问题, 本发明是这样实现的:
两相流体回路真空热性能试验装置包括: 散热板、 控溫加热器、 多层隔热 组件、 温度传感器、 模拟热源和回路支架; 其中, 散热板通过隔热垫隔热安装 在回路支架的上部; 两相流体回路的冷凝管路埋在散热板中, 两相流体回路的 储液器半埋在散热板中; 两相流体回路中的蒸发器隔热安装在回路支架的下部; 控温加热器安装在两相流体回路的蒸汽管路、 储液器、 控制阀和液体管路上; 温度传感器安装在两相流体回路的蒸发器、 蒸汽管路、 冷凝管路、 储液器、 控 制阀和液体管路、 模拟热源以及散热板边缘区域上; 多层隔热組件包裹在蒸汽
管路、 储液器、 控制阀和液体管路上; 模拟热源为 RHU同位素电模拟热源, 固 定安装在蒸发器内; 安装为散热板提供工作温度的散热板加热器, 所述散热板 加热器为安装在散热板外侧空间的红外加热器或粘贴在散热板上的加热片; 回 路支架放置在真空仓中;
其中, 所述蒸发器安装在隔热板上, 模拟热源放置在蒸发器的内部, 模拟 热源工装的耳片通过螺 和隔热垫固定在隔热板上, 所迷隔热板通过 4 个隔热 柱固定安装在回路支架上;
模拟热源用于控制蒸发器的温度,使蒸发器的温度为 -55°C〜50°C;散热板加 热器用于控制散热板的温度,使散热板的温度为 -60°C~50°C; 控温加热器用于防 止蒸汽管路、 储液器、 控制阀和液体管路冻结, 控温加热器的自控门限设置为 -55°C~-30°C;
所述温度传感器用于观察重力驱动两相流体回路中氨工质在各部件中的状 态, 温度传感器的安装位置为:
蒸发器的 4个翅片上沿高度方向分别布置至少 2个温度传感器, 其中一个 位于蒸发器翅片的下端, 一个位于蒸发器翅片的上端;
蒸气管路的进口、 顶部和出口处分别布置 1个温度传感器;
冷凝管路的进口、 出口分别布置 1 个温度传感器, 在冷凝管路的翅片上布 置至少 1个温度传感器;
储液器的外表面沿高度方向布置 3 个温度传感器, 分别位于储液器的气空 间、 气液界面和液体空间;
连接储液器和控制阀的液体管路上布置至少 1 个温度传感器, 在连接控制 阀和蒸发器的液体管路上布置至少 1个温度传感器;
控制阀上布置 1个温度传感器;
模拟热源上布置至少 1个温度传感器;
散热板的内表面的边缘区域布置至少 1个温度传感器。
其中, 所述隔热板 (12)、 隔热垫 (13) 和隔热柱 (14) 材料为聚酰亚胺或 玻璃钢。
所述散热板(11 ) 的基板为铝板或蜂窝板, 散热板(11 ) 的表面粘贴有 OSR 片或喷涂高发射率的涂层。
所述控温加热器为加热片、 加热丝、 加热带或加热板。
本发明还提供了一种采用上述试验装置的两相流体回路真空热性能试验方 法, 能够对两相流体回路在不同工作温度下的传热能力和阻断性能进行测试、 评估。
所迷试验方法包括如下步骤:
步骤 2 , 将回路支架放入真空仓中, 抽真空, 使得真空度小于 2x l (T3Pa, 设 置储液器、 控制阀、 液体管路和蒸气管路上的控温加热器为自控状态, 自控门 限为 -55° (:〜 -30°C; 设置散热板加热器的自控门限为 -55°C~-30°C;
步骤 3, 向真空仓的热沉通液氮, 降低真空仓温度至 -150°C; 将储液器的温 度降至第一测试温度 -50°C, 且达到两相流体回路工况平衡; 所迷工况平衡为储 液器温度在半小时维持不变或单调变化小于 l °C/h ; 储液器的温度即为两相流体 回路的工作温度;
步骤 4, 极限传热能力测试:
开启模拟热源, 按照设定的步长增加模拟热源的加热功率, 在每次增加模 拟热源的加热功率的同时减小散热板加热器的加热功率, 使储液器的温度维持 在 -50°C, 且达到两相流体回路工况平衡, 直至散热板加热器的加热功率为零或 者因蒸发器的温度突升导致无法维持工况平衡; 则散热板加热器的加热功率为
零时或者蒸发器的温度突升前一平衡时刻的模拟热源的加热功率即为该工作温 度下两相流体回路的极限传热能力;
步骤 5 , 通过降低蒸发器的功率、 同时增加散热板的功率, 改变储液器的温 度至各测试温度, 依照步骤 4 的方法, 获得各测试温度下两相流体回路的极限 传热能力, 其中, 按照递升的方式改变储液器温度;
步骤 6 , 两相流体回路阻断能力测试:
不同工作温度下, 当两相流体回路运行在平衡工况时, 保持模拟热源和散 热板加热器的加热功率不变, 对控制阀进行开关操作, 检查两相流体回路的阻 断性能: 如果关闭控制阀后, 蒸发器的温度不断升高后突升、 散热板的温度不 断降低, 而重新开启控制阀后, 蒸发器温度降低、 散热板温度提升, 直至达到 工况平衡, 表明两相流体回路阻断性能正常; 如果关闭控制阀后, 蒸发器的温 度不变或平稳升高, 则表明两相流体回路阻断性能不正常。
其中, 所述步骤 3的降温过程中, 开启模拟热源, 使得两相流体回路运行, 加快蒸发器的降温速率。
有益效果:
( 1 ) 采用本发明试验装置和试验方法可对两相流体在真空环境下的传热和 阻断性能进行全面、 有效的评估。
(2) 散热板的基板选为铝板或蜂窝板, 在其表面粘贴 OSR 片或喷涂高发 射率的涂层, 有利于提高散热板的散热率。
(3 ) 温度传感器的布置有利于观察两相流体回路中氨工质的状态, 查看两 相流体回路中的各部件是否满足温度要求, 同时还可以查看两相流体回路是否 达到平衡。
(4) 由于冷凝管路和蒸发器降温速率不同, 在降温过程中加大模拟热源的
加热功率可以使得蒸发器的温度提升, 两相流体回路中的氨工质将蒸发器的热 量传递至冷凝管路, 能够提高蒸发器的降温速率。 附图说明
图 1 为重力驱动两相流体回路系统组成示意图。
图 2为两相流体回路真空热性能试验装置示意图。
图 3为两相流体回路蒸发器的安装示意图。
图 4为两相流体回路上的温度传感器的布置示意图。
图 5为散热板 (包括冷凝管路) 上温度传感器的布置示意图。
其中, 1 -蒸发器, 2-蒸汽管路, 3-冷凝管路, 4-储液器, 5-控制阀, 6-液体 管路, 7-丝网蒸发器, 8-液体分流器, 9-蒸汽汇流器, 〗0-真空仓, 1 1-散热板, 12-隔热板, 13-隔热垫, 14-隔热柱, 15-模拟热源, 16-红外加热器, 17-回路支 架。 具体实施方式
下面结合附图并举实施例, 对本发明进行详细描述。
本发明提供了一种两相流体回路真空热性能试验装置, 如图 2 所示, 包括 散热板 1 1、 控温加热器、 多层隔热組件、 温度传感器、 模拟热源 15和回路支架 17。
其中, 两相流体回路和散热板 1 1 隔热安装在回路支架 17上, 散热板 1 1 用 隔热垫隔热安装在回路支架 Π的上部,用于模拟两相流体回路在轨的散热部分; 两相流体回路的冷凝管路 3埋在散热板 11 中, 两相流体回路的储液器 4半埋在 散热板 1 1 中, 位于冷凝管路 3的出口处; 两相流体回路中的蒸发器 1 隔热安装
在回路支架 17的下部, 位于冷凝管路 3的下方; 控温加热器安装在两相流体回 路的蒸汽管路 2、 储液器 4、 控制阀 5和液体管路 6上, 防止管路冻结; 温度传 感器安装在两相流体回路的蒸发器 1、 蒸汽管路 2、 冷凝管路 3、 储液器 4、 控 制阀 5和液体管路 6 , 以及散热板 11 上, 用于测量两相流体回路各部件以及散 热板的温度, 检测两相流体回路的运行情况; 多层隔热組件安装在蒸汽管路 2、 储液器 4、 控制阀 5和液体管路 6上, 用来防止管路部分环境漏热, 模拟在轨工 况; 模拟热源 15采用 RHU同位素电模拟热源, 固定安装在蒸发器 1 内, 用来 模拟同位素加热器件, 模拟热源 15同时也是蒸发器 1 的控温加热器; 回路支架 17放置在真空仓 10 中, 真空仓 10提供温度不大于 80K, 真空度小于 2x l(T3pa 的真空环境。
其中, 散热板的基板可以采用铝板或蜂窝板等导热性能较好的材料制成, 其外表面粘贴有 OSR片, 或喷涂高发射率的涂层, 从而有利于散热。
蒸发器 1、 模拟热源 15与回路支架 17之间的隔热方式如图 3所示, 蒸发器 1安装在隔热板 12上, 模拟热源 15放置在蒸发器 1 的内部, 模拟热源 15工装 的耳片通过螺钉和隔热垫 13 固定在隔热板 12上, 所述隔热板 12通过 4个隔热 柱 14固定安装在回路支架 17上。 其中, 隔热板 12、 隔热垫 13和隔热柱 14材 料为聚酰亚胺或玻璃钢等导热率低的材料。 液体分流器 8下表面与隔热板 12上 表面间的距离大于 10mm, 隔热板 12 与回路支架 17 间的有效隔热距离大于 100mm , 隔热垫 13的外径小于 10mm。
温度传感器为热电偶温度传感器, 其布置如图 4 所示。 在两相流体回路上 布置 34个溫度传感器:
①在蒸发器 1 的 4个翅片上沿高度方向由下至上分别均匀布置 3 个温度传 感器, 共 12 个, 编号 T1~T12 , 也可以只在蒸发器翅片的下端和上端布置传感
器, 主要是用于测量蒸发器中液态工质和气态工作的温度, 从而反应蒸发器 1 的工作状态。
②在蒸气管路 2 的进口、 顶部和出口处分别布置 1 个温度传感器, 编号分 别为 T13、 T14和 Τ15。
③在冷凝管路 3 的进口、 出口及冷凝管路上布置 9 个温度传感器, 编号 T16-T24 , 如图 5所示; 冷凝管路 3—般安装有翅片, 用于增大散热面积, 温度 传感器一般安装在翅片上。
④在储液器 4 的外表面沿高度方向布置 3 个温度传感器, 编号 Τ25 Τ27 , 分别用于测量储液器 4中气体、 气液界面和液体的温度。
⑤液体管路 6分为两段,一段连接储液器 3和控制阀 5, 另一段连接控制阀 5和蒸发器 1。 其中, 在连接储液器 3和控制阀 5的液体管路的中点处布置 1个 溫度传感器, 编号 Τ28 ;在连接控制阀 5和蒸发器 1 的液体管路的进口和出口处 分别布置 1 个温度传感器, 编号分别为 T31 和 Τ32 , 也可以在连接控制阀 5和 蒸发器 1的液体管路的中点处布置 1个温度传感器。
⑥在控制阀 5上布置温度传感器。若控制阀 5由两个并行的阀(a阀和 b阀) 组成, 则在 a阀和 b阀上分别布置 1个温度传感器, 编号分别为 T29和 T30 ;
⑦在模拟热源上布置 2个温度传感器, 编号为 T33和 T34 ;
⑧在散热板 11 的内表面的边缘区域布置 4 个温度传感器, 编号为 T35 和 T38 , 4个温度传感器距散热板边缘 100mm, 如图 5所示。
温度传感器所在位置即为测点位置。
控温加热器可以是加热片、 加热丝、 加热带、 加热板或其他加热方式, 采 用 PID控制或通断控温的方式, 主要是防止两相流体回路各部件被冻结。 其中, 储液器 4上的控温加热器采用在储液器 4上串联安装 2个加热片实现;控制阀 5
上的控温加热器采用在控制阀 5 连接的液体管路上安装加热带, 如图 2所示的 (测点 28和测点 29之间管路、 测点 29与测点 31之间管路、 测点 28与测点 30 之间管路、侧点 30与测点 31之间管路)分别安装 1个加热带, 4个加热带串联, 每段管路长约 50mm ; 液体管路 6 上的控温加热器采用在液体管路 6上的测点 3 1与测点 32之间安装 1个加热带实现;蒸气管路 2上的控温加热器采用 3个串 联安装的加热带实现。
储液器 4、 控制阀 5、 液体管路 6和蒸气管路 2上的控温加热器主要起防止 管路冻结的作用。
蒸发器 1的温度控制依靠安装在其内部的模拟热源 15实现。 由于在传热过 程中, 同位素热源的热量被两相流体回路传递带走, 同位素热源自身表面的温 度会降低到与蒸发器的温度一致。
冷凝管路 2预埋在散热板 1 1 中, 与散热板 1 1 的温度基本一致, 散热板 11 的温度控制依靠安装在散热板 1 1 外側的红外加热器 16 或者是粘贴在散热板上 的加热片实现。
其中, 控制散热板 11 的温度为 -60°C~50°C。 由于两相流体回路运行过程中 氨工质的热传递作用, 蒸发器 1、 蒸汽管路 2、 冷凝管路 3、 储液器 4、 控制阀 5 和液体管路 6的温度基本在 -55°C〜50° (:范围内。其中,储液器 4的温度即为两相 流体回路的工作温度。
选择测点 T1 (蒸发器 1下部, 靠近液体管路 6的出口)、 T3 (蒸发器 1上部, 靠近蒸 气管路 2的进口)、 T14 (蒸气管路 2中部)、 T17 (冷凝管路 3进口)、 T23 (冷凝管路 3出 口)、 T25 (储液器 4上部, 即储液器气空间)、 T27 (储液器下部)、 T29-T30 (控制阀 a和 控制阀 b)、 T3 1 (液体管路 6进口)、 T35-T38 (散热板 11的 4个角) 为温度监测 点, 监控模拟热源 15、 散热板 11和两相流体回路是否满足温度要求, 同时, 通
过比较温度监测点与其他测点的温度, 判断是否达到平衡。
利用上述试验装置进行重力驱动两相流体回路真空热性能试验, 测试重力 驱动两相流体回路在不同的工作温度下的极限传热性能和阻断性能。 其中, 两 相流体回路的工作温度为储液器 4 的温度, 测试过程中, 依靠改变蒸发器 1 和 散热板 11 的温度改变储液器 4的温度, 储液器 4、 控制阀 5、 液体管路 6和蒸 气管路 2 上的控溫加热器仅用于防止两相流体回路中各部件被冻结, 具体实现 步骤如下:
步骤 1, 将回路支架 17放入真空仓 10中, 抽真空 (真空度小于 2xl0_3pa), 设置储液器 4、控制阀 5、液体管路 6和蒸气管路 2上的控温加热器为自控状态, 自控门限为 -55°C〜- 30°C, 即当温度小于自控门限时, 控温加热器自动开启, 防 止其被冻结。 设置散热板加热器的自控门限为 -55°C— 30t。
步骤 2 , 向真空仓的热沉通液氮, 降低真空仓温度至 -150°C, 由于两相流体 回路的蒸汽管路 (2)、 储液器 (4)、 控制阀 (5) 和液体管路 (6) 被多层隔热 組件包裹, 其降温速率慢, 散热板的降温速率最快, 为提高两相流体回路各部 件的降温速率, 在降温过程中, 开启模拟热源 15 , 使得两相流体回路运行, 通 过散热板中的冷凝管路带动蒸发器、 储液器降温, 加快蒸发器的降温速率, 直 到将储液器的温度降至 -50°C, 当储液器温度在半小时維持不变或单调变化小于 l°C/h时, 认为工况平衡。 储液器的温度即为两相流体回路的工作温度。
步骤 3, 极限传热能力测试: 按照一定的步长增加蒸发器的加热功率 (即模 拟热源的加热功率), 在每次增加模拟热源的加热功率的同时同步减小散热板加 热器的加热功率, 使储液器的温度维持在 -50°C , 每次加热功率调整后均需等待 两相流体回路工况平衡, 直至散热板加热器的加热功率为零或者因蒸发器的温 度突升导致无法维持工况平衡。 当散热板加热功率为 0 时, 散热板达到此工作
温度下的最大散热能力, 蒸发器加热功率的继续提升会使得储液器的温度升高, 不能继续維持在 -50°C。当蒸发器的加热功率大于两相流体回路极限传热能力时, 蒸发器内的液体被烧干, 导致蒸发器的温度突升。 因此, 散热板加热器的加热 功率为零时或者蒸发器的温度突升前一平衡时刻的蒸发器的加热功率为该工作 温度下两相流体回路的极限传热能力。
步驟 4 , 通过降低蒸发器的功率、 同时增加散热板的功率, 改变储液器的温 度, 依照步骤 3 的方法, 获得不同工作溫度下两相流体回路的极限传热能力。 其中, 在测试不同工作温度下两相流体回路的极限传热能力时, 工作温度的调 整方法为逐步升高, 如首先测 -50°C工作温度时的极限传热能力, 然后依次测量 -40°C、 -30°C、 -20°C……工作温度时的极限传热能力。
步骤 5, 两相流体回路阻断能力测试:
不同工作温度下, 当两相流体回路运行在平衡工况时, 保持蒸发器和散热 板加热器的加热功率不变, 对重力驱动两相流体回路的阀进行开关操作, 检查 两相流体回路的阻断性能: 如果关闭控制阀后, 蒸发器的温度不断升高并迅速 突升, 散热板的温度不断降低, 重新开启控制阀, 蒸发器温度降低、 散热板温 度提升, 直至达到工况平衡, 表明两相流体回路阻断性能正常; 如果关闭控制 阀后, 蒸发器的温度不变或緩慢升高, 则表明两相流体回路阻断性能不正常。
综上所述, 以上仅为本发明的较佳实施例而已, 并非用于限定本发明的保 护范围。 凡在本发明的精神和原则之内, 所作的任何修改、 等同替换、 改进等, 均应包含在本发明的保护范围之内。
Claims
1、一种两相流体回路真空热性能试验装置,其特征在于,包括:散热板(11)、 控温加热器、 多层隔热組件、 温度传感器、 模拟热源 (15) 和回路支架 (17); 其中, 散热板 (11) 通过隔热垫隔热安装在回路支架 (17) 的上部; 两相流体 回路的冷凝管路 (3) 埋在散热板 (11) 中, 两相流体回路的储液器 (4) 半埋 在散热板 (11) 中; 两相流体回路中的蒸发器 (1) 隔热安装在回路支架 (17) 的下部; 控温加热器安装在两相流体回路的蒸汽管路 (2)、 储液器 (4)、 控制 阀 (5) 和液体管路 (6) 上; 温度传感器安装在两相流体回路的蒸发器 (1)、 蒸汽管路 (2)、 冷凝管路 (3)、 储液器 (4)、 控制阀 (5) 和液体管路 (6)、 模 拟热源 (15) 以及散热板(11) 边缘区域上; 多层隔热组件包裹在蒸汽管路(2)、 储液器 (4)、 控制阀 (5) 和液体管路 (6) 上; 模拟热源 (15) 为 RHU同位素 电模拟热源, 固定安装在蒸发器 (1) 内; 安装为散热板 (11) 提供工作温度的 散热板加热器, 所述散热板加热器为安装在散热板外侧空间的红外加热器 (16) 或粘贴在散热板上的加热片; 回路支架 (17) 放置在真空仓 (10) 中;
其中, 所述蒸发器 (1) 安装在隔热板 (12) 上, 模拟热源 (15) 放置在蒸 发器 (1) 的内部, 模拟热源 (15) 工装的耳片通过螺钉和隔热垫 (13) 固定在 隔热板 (12) 上, 所述隔热板 (12) 通过 4 个隔热柱 (14) 固定安装在回路支 架 (17) 上;
模拟热源(15)用于控制蒸发器的温度,使蒸发器(1)的温度为 -55 5(TC; 散热板加热器用于控制散热板(11)的温度,使散热板(11)的温度为 -60°C~50°C; 控温加热器用于防止蒸汽管路 (2)、 储液器 (4)、 控制阀 (5) 和液体管路 (6) 冻结, 控温加热器的自控门限设置为 -55°C〜- 30' (:。
2、 如权利要求 1所述的两相流体回路真空热性能试验装置, 其特征在于,
所述温度传感器的安装位置为:
蒸发器 (1 ) 的 4个翅片上沿高度方向分别布置至少 2个温度传感器, 其中 一个位于蒸发器翅片的下端, 一个位于蒸发器翅片的上端;
蒸气管路 (2) 的进口、 顶部和出口处分别布置 1个溫度传感器; 冷凝管路 (3) 的进口、 出口分别布置 1 个温度传感器, 在冷凝管路 (3 ) 的翅片上布置至少 1个温度传感器;
储液器(4) 的外表面沿高度方向布置 3个温度传感器,分别位于储液器(4) 的气空间、 气液界面和液体空间;
连接储液器 (3 ) 和控制阀 (5 ) 的液体管路上布置至少 1 个温度传感器, 在连接控制阀 (5 ) 和蒸发器 (1 ) 的液体管路上布置至少 1个温度传感器; 控制阀 (5) 上布置 1个温度传感器;
模拟热源 (15 ) 上布置至少 1个温度传感器;
散热板 (11 ) 的内表面的边缘区域布置至少 1个温度传感器。
3、 如权利要求 1所述的两相流体回路真空热性能试验装置, 其特征在于, 所述隔热板 (12)、 隔热垫 (13 ) 和隔热柱 (14) 材料为聚酰亚胺或玻璃钢。
4、 如权利要求 1所述的两相流体回路真空热性能试验装置, 其特征在于, 所述散热板 (11 ) 的基板为铝板或蜂窝板, 散热板 (11 ) 的表面粘贴有 OSR片 或喷涂高发射率的涂层。
5、 如权利要求 1所述的两相流体回路真空热性能试验装置, 其特征在于, 所述控温加热器为加热片、 加热丝、 加热带或加热板。
6、 一种采用如权利要求 1~5任意一项所述的试验装置的两相流体回路真空 热性能试验方法, 其特征在于, 包括如下步骤:
步骤 1 , 将回路支架 (17) 放入真空仓 (10) 中, 抽真空, 使得真空度小于
2x l O-3Pa, 设置储液器 (4)、 控制阀 (5)、 液体管路 (6) 和蒸气管路 (2) 上的 控温加热器为自控状态, 自控门限为 -55°C〜- 30°C; 设置散热板加热器的自控门 限为 -55°C〜- 30°C;
步骤 2, 向真空仓 (10) 的热沉通液氮, 降低真空仓温度至 -150°C ; 将储液 器的温度降至第一测试温度 -50°C , 且达到两相流体回路工况平衡; 所述工况平 衡为储液器温度在半小时维持不变或单调变化小于 l °C/h ; 储液器的温度即为两 相流体回路的工作温度;
步骤 3, 极限传热能力测试:
开启模拟热源, 按照设定的步长增加模拟热源的加热功率, 在每次增加模 拟热源的加热功率的同时减小散热板加热器的加热功率 > 使储液器的温度维持 在 -50Ό , 且达到两相流体回路工况平衡, 直至散热板加热器的加热功率为零或 者因蒸发器的温度突升导致无法维持工况平衡; 则散热板加热器的加热功率为 零时或者蒸发器的温度突升前一平衡时刻的模拟热源的加热功率即为该工作溫 度下两相流体回路的极限传热能力;
步骤 4, 通过降低蒸发器的功率、 同时增加散热板的功率, 改变储液器的温 度至各测试温度, 依照步骤 3 的方法, 获得各测试温度下两相流体回路的极限 传热能力, 其中, 按照递升的方式改变储液器温度;
步骤 5, 两相流体回路阻断能力测试:
不同工作温度下, 当两相流体回路运行在平衡工况时, 保持模拟热源和散 热板加热器的加热功率不变, 对控制阀进行开关操作, 检查两相流体回路的阻 断性能: 如果关闭控制阀后, 蒸发器的温度不断升高后突升、 散热板的温度不 断降低, 而重新开启控制阀后, 蒸发器温度降低、 散热板温度提升, 直至达到 工况平衡, 表明两相流体回路阻断性能正常; 如果关闭控制阔后, 蒸发器的温
度不变或平稳升高, 则表明两相流体回路阻断性能不正常。
7、 如权利要求 6所述的两相流体回路真空热性能试验方法, 其特征在于, 所述步骤 2的降温过程中, 幵启模拟热源 (15 ), 使得两相流体回路运行, 加快 蒸发器 (1 ) 的降温速率。
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